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G4RDAtomicTransitionManager.hh
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26 //
27 // $Id: G4RDAtomicTransitionManager.hh,v 1.2 ????
28 // GEANT4 tag $Name: geant4-09-01-ref-00 $
29 //
30 // Authors: Elena Guardincerri (Elena.Guardincerri@ge.infn.it)
31 // Alfonso Mantero (Alfonso.Mantero@ge.infn.it)
32 //
33 // History:
34 // -----------
35 //
36 // 16 Sept 2001 EG Modified according to a design iteration in the
37 // LowEnergy category
38 //
39 // -------------------------------------------------------------------
40 
41 // Class description:
42 // Low Energy Electromagnetic Physics: create or fills and manages G4RDAtomicShell,
43 // G4RDFluoTransition, G4RDAugerTransition objects.
44 // Further documentation available from http://www.ge.infn.it/geant4/lowE
45 
46 // -------------------------------------------------------------------
47 
48 #ifndef G4RDAtomicTransitionManager_h
49 #define G4RDAtomicTransitionManager_h 1
50 
51 #include "G4RDShellData.hh"
52 #include "G4RDFluoData.hh"
53 #include "G4RDAugerData.hh"
54 #include "G4RDFluoTransition.hh"
55 #include "G4RDAtomicShell.hh"
56 // #include "g4std/map"
57 #include <vector>
58 #include "globals.hh"
59 
60 // This class is a singleton
62 
63 public:
64 
65  // The only way to get an instance of this class is to call the
66  // function Instance()
68 
69  // Z is the atomic number of the element, shellIndex is the
70  // index (in EADL) of the shell
71  G4RDAtomicShell* Shell(G4int Z, size_t shellIndex) const;
72 
73  // Z is the atomic number of the element, shellIndex is the
74  // index (in EADL) of the final shell for the transition
75  // This function gives, upon Z and the Index of the initial shell where te vacancy is,
76  // the radiative transition that can happen (originating shell, energy, probability)
77  const G4RDFluoTransition* ReachableShell(G4int Z, size_t shellIndex) const ;
78 
79  // This function gives, upon Z and the Index of the initial shell where te vacancy is,
80  // the NON-radiative transition that can happen with originating shell for the transition, and the
81  // data for the possible auger electrons emitted (originating vacancy, energy amnd probability)
82 
83  const G4RDAugerTransition* ReachableAugerShell(G4int Z, G4int shellIndex) const ;
84 
85  // This function returns the number of shells of the element
86  // whose atomic number is Z
87  G4int NumberOfShells(G4int Z) const;
88 
89  // This function returns the number of those shells of the element
90  // whose atomic number is Z which are reachable through a radiative
91  // transition
92 
93  // This function returns the number of possible radiative transitions for the atom with atomic number Z
94  // i.e. the number of shell in wich a vacancy can be filled with a radiative transition
95 
97 
98 // This function returns the number of possible NON-radiative transitions for the atom with atomic number Z
99 // i.e. the number of shell in wich a vacancy can be filled by a NON-radiative transition
100 
102 
103  // Gives the sum of the probabilities of radiative transition towards the
104  // shell whose index is shellIndex
105  G4double TotalRadiativeTransitionProbability(G4int Z, size_t shellIndex);
106 
107  // Gives the sum of the probabilities of non radiative transition from the
108  // shell whose index is shellIndex
110 
111 protected:
112 
113  G4RDAtomicTransitionManager(G4int minZ = 1, G4int maxZ = 100,
114  G4int limitInfTable = 6, G4int limitSupTable=100 );
116 
117 private:
118  // Hide copy constructor and assignment operator
121 
123 
124  // the first element of the map is the atomic number Z.
125  // the second element is a vector of G4RDAtomicShell*.
126  std::map<G4int,std::vector<G4RDAtomicShell*>,std::less<G4int> > shellTable;
127 
128  // the first element of the map is the atomic number Z.
129  // the second element is a vector of G4AtomicTransition*.
130  std::map<G4int,std::vector<G4RDFluoTransition*>,std::less<G4int> > transitionTable;
131 
132  // since Augereffect data r stored as a table in G4RDAugerData, we have here a pointer to an element of that class itself.
133 
135 
136  // Minimum and maximum Z in EADL table containing identities and binding
137  // energies of shells
140 
141  // Minimum and maximum Z in EADL table containing identities, transition
142  // energies and transition probabilities of shells
145 
146 
147 };
148 
149 #endif
G4RDAtomicTransitionManager & operator=(const G4RDAtomicTransitionManager &right)
G4double TotalNonRadiativeTransitionProbability(G4int Z, size_t shellIndex)
static const G4int maxZ
Float_t Z
double G4double
Definition: G4Types.hh:76
const G4RDAugerTransition * ReachableAugerShell(G4int Z, G4int shellIndex) const
static G4RDAtomicTransitionManager * Instance()
std::map< G4int, std::vector< G4RDFluoTransition * >, std::less< G4int > > transitionTable
std::map< G4int, std::vector< G4RDAtomicShell * >, std::less< G4int > > shellTable
G4RDAtomicShell * Shell(G4int Z, size_t shellIndex) const
int G4int
Definition: G4Types.hh:78
G4RDAtomicTransitionManager(G4int minZ=1, G4int maxZ=100, G4int limitInfTable=6, G4int limitSupTable=100)
static G4RDAtomicTransitionManager * instance
const G4RDFluoTransition * ReachableShell(G4int Z, size_t shellIndex) const
G4double TotalRadiativeTransitionProbability(G4int Z, size_t shellIndex)
G4int NumberOfReachableAugerShells(G4int Z) const